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. Author manuscript; available in PMC: 2022 Mar 1.
Published in final edited form as: Appl Opt. 2021 Dec 20;60(36):11189–11195. doi: 10.1364/AO.443972

Fig. 3.

Fig. 3.

Dynamic wavefront distortions at various deflection angles in a galvanometric resonant scanner with a SiC mirror oscillating at 13.8 kHz and over a 4 mm clear aperture diameter, (a) Full wavefront, and (b) after oblique astigmatism subtraction; (c) and (d) show the linear increase of wavefront P-V and RMS with beam deflection angle. The dotted lines parallel to the x axis in (d) represent diffraction-limited RMS for the corresponding wavelengths. The Strehl ratio as a function of the beam deflection angle at 450, 650 and 850 nm wavelengths is shown in (e), and the green shaded region satisfies Maréchal diffraction-limited performance. The values along the top horizontal axes in light orange denote the Lagrange invariant (product of maximum peak-to-peak beam deflection angle and beam diameter) in units of millimeters/degrees to facilitate performance comparison with other scanners.